The kinetic molecular theory of gases tells us about the **kinetic equation** for gases. This theory also explains the kinetic energy of gases and on what factor the kinetic energy of ideal gas depends. The kinetic molecular theory of gases is completely valid for ideal gases but, partially valid for non-ideal gases or real gases. Here’s some scientists and his contribution are given below:

**Bernoulli (1738):**Founder of the kinetic molecular theory of gases.**Clausius (1857):**Derive**kinetic equation**and deduced all the gas laws from KMT.**Maxwell:**Presented the law of distribution of velocities.**Ven der Waal:**Corrected the pressure and volume factor in ideal gas equation to make it applicable to the real gases.

Before we derive the **kinetic equation,** it’s very important to understand the postulates of the kinetic molecular theory of gases.

## Postulates of Kinetic Molecular Theory

- Gas is made up of small particles called atom or molecules. Gases like helium, neon, argon have mono-atomic molecules.
- Molecules of small gas are identical in all respects (having same mass, shape, and size).
- Molecules are constantly in random motion along straight line. (assumption)

Let a molecule of gas is moving with speed u. The components of u are in three directions u_{x}, u_{y}, and u_{z}.

It assumes that the probability of movement of a gas molecule in X-direction, Y-direction, and Z-direction is the same so,

u_{x} = u_{y} = u_{z}

The magnitude of** **u:

u = u_{x} i + u_{y} j + u_{z} k

u = √u_{x}^{2} + u_{y}^{2} + u_{z}^{2}

u^{2} = u_{x}^{2} + u_{y}^{2} + u_{z}^{2}

If; u_{x} = u_{y} = u_{z}

**u ^{2} = 3u_{x}^{2}**

4. All the collisions of gas molecules among themselves and with the wall of the container are** elastic in nature**. Elastic in nature means there is no loss in momentum (momentum remains conserved) and kinetic energy (kinetic energy remains the same before and after collision).

5. The pressure of a gas is due to the collision of molecules with the wall of the container.

We have a container containing a gas molecule, a molecule of gas is move with momentum mv:

When a gas molecule collides with the wall of the container, its momentum is changed (-mv). The momentum of a gas molecule is the same but opposite in direction. The gas molecule exerts a force on the wall of the container and change in momentum is due to force so, the force exerted by a gas molecule per unit area is called** pressure.** The more the number of molecules collides, the more will be the pressure.

6. The kinetic energy of gas (ideal) depends only and only upon absolute temperature. The kinetic energy of gas does not depend upon the nature of the gas. It also does not depend upon the pressure.

The nature of gas means if we take one mole of hydrogen gas (ideal) and 1 mole of Oxygen gas (ideal) at 27 degrees Celsius, the kinetic energy of the gas is the same.

7. The volume occupied by gas molecules is negligible when compared to the volume of gas. (assumption)

8. There is no intermolecular force of attraction among molecules. (assumption)

9. There is no effect of gravity on the motion of the molecules of a gas.

## Kinetic Equation for Gases

On the basis of kinetic theory, it is possible to derive a relation between the pressure and volume of gas in the form of an equation.

PV = 1/3 mn u_{rms}^{2}

Where,

- P = Pressure
- V = Volume
- m = mass of one molecule of gas
- n = number of molecules
- u
_{rms}^{2}= Root mean square velocity of molecules

**What is u _{rms}^{2}?**

Let us have an nth number of gas particles having different velocities u_{1}, u_{2}, u_{3},…, u_{n}.

u = u_{1} + u_{2} + u_{3} + …… + u_{n}

Squaring both sides

u^{2} = u_{1}^{2} + u_{2}^{2} + u_{3}^{2} + …… + u_{n}^{2}

Taking average (mean)

u^{2} = u_{1}^{2} + u_{2}^{2} + u_{3}^{2} + …… + u_{n}^{2} / N

where, N = total number of molecules

Taking under root both sides

√u^{2} = √u_{1}^{2} + u_{2}^{2} + u_{3}^{2} + …… + u_{n}^{2} / N

u_{rms }= √u_{1}^{2} + u_{2}^{2} + u_{3}^{2} + …… + u_{n}^{2} / N

This is called **root mean square velocity.**

## Derivation of Kinetic Equation For Gases

Let we have a gas container having n number of gas molecules of direction x, y, and z, and length L.

Consider a small molecule of a gas with mass m and velocity u_{1}. As we know that the velocity of a molecule having three components but we assume only u_{x }component and we are also considered only one side of the container which is also along x-direction.

**How to pressure exerted**** ****by a small molecule of gas when collied with the wall of the container?**

- The collision of gas molecule is elastic so kinetic energy remain same. (Before and after collision)
- The momentum is changed.

### Change in Momentum in Each Collision

Intial momentum = P_{i} = mu_{x1}

Final momentum = P_{f} = -mu_{x1}

Chamge in momentum = Intial momentum – Final momentum

△P = mu_{x1} – (- mu_{x1})

△P = 2mu_{x1} (△P in each collision)

The change in momentum is due to force

### Time Taken For Each Collision

As the length of the side is “L” and the speed of the molecule is u_{x1}.

**Before collision:**molecule of a gas is moved toward a wall of the container.**After collision:**molecule of a gas is moved away from a wall of the container.

So, the total length is 2L.

time = distance / speed

time = 2L / u_{x1} (time taken for each collision)

### Force Exerted on the Wall

Force exerted on wall = △P / △t = change in momentum / change in time

putting the values of △P and △t

Force exerted on wall = 2mu_{x1} / 2L / u_{x1}

Force exerted on wall = 2mu_{x1} × u_{x1} / 2L

Force exerted on wall = mu_{x1}^{2} / L ——- (1)

(Force applied on the wall by one molecule due to collision)

If we want to write in terms of u, then

u = u_{x} i + u_{y} j + u_{z} k

u_{x} = u_{y} = u_{z}

u^{2} = u_{x}^{2} i + u_{y}^{2} j + u_{z}^{2} k

u^{2} = 3u_{x}^{2}

u_{1}^{2} = 3u_{x1}^{2}

u_{x1}^{2} = 1/3 u_{1}^{2}

Put in eq (1)

Force exerted on wall = m/L × 1/3 u_{1}^{2}

Force exerted on wall = m/3L × u_{1}^{2} (Force due to one molecule)

#### Force due to two molecules

F_{2}= m/3L × u_{2}^{2}

#### Force due to three molecules

F_{3}= m/3L × u_{3}^{2}

#### Force due to nth molecules

F_{n}= m/3L × u_{n}^{2}

F_{net} = F_{1} + F_{2} + F_{3} + …… + F_{n}

F_{net} = m/3L × u_{1}^{2} + m/3L × u_{2}^{2} + m/3L × u_{3}^{2} + ….. + m/3L × u_{n}^{2}

F_{net} = m/3L ( u_{1}^{2} + u_{2}^{2} + u_{3}^{2} + ….. + u_{n}^{2})

Multiply and divided bt “n”

F_{net} = m/3L ( u_{1}^{2} + u_{2}^{2} + u_{3}^{2} + ….. + u_{n}^{2} / n) × n

As, u_{rms }= √u_{1}^{2} + u_{2}^{2} + u_{3}^{2} + …… + u_{n}^{2} / N

u_{rms}^{2}= u_{1}^{2} + u_{2}^{2} + u_{3}^{2} + …… + u_{n}^{2} / N

F_{net} = mn/3L × u_{rms}^{2}

As,

Pressure = Force / Area

Pressure = mn/3L × u_{rms}^{2} / A

Pressure = mn u_{rms}^{2} / 3L A

As, A = L × W = L × L = L^{2}

P = mn u_{rms}^{2} / 3L × L^{2}

P = mn u_{rms}^{2} / 3L^{3}

As, L^{3} = volume of cylinder = L × W × h = L × L × L = L^{3}

P = mn u_{rms}^{2} / 3 V

**PV = 1/3 mn u _{rms}^{2} **

This is called **Kinetic equation **for gases.

PV = 1/3 mn u_{rms}^{2} ——– (1)

As we know that the kinetic energy is equal to 1/2 mv^{2}

K.E of one molecule = 1/2 mu_{1}^{2}

K.E of two molecules = 1/2 mu_{2}^{2}

K.E of three molecules = 1/2 mu_{3}^{2}

K.E of nth molecules = 1/2 mu_{n}^{2}

K.E of n molecules = 1/2 mu_{1}^{2} + 1/2 mu_{2}^{2} + 1/2 mu_{3}^{2} + …… + 1/2 mu_{n}^{2}

K.E of n molecules = 1/2 m (u_{1}^{2} + u_{2}^{2} + u_{3}^{2} + …… + u_{n}^{2} )

K.E of n molecules = 1/2 m (u_{1}^{2} + u_{2}^{2} + u_{3}^{2} + …… + u_{n}^{2} / n) × n

K.E of n molecules = 1/2 mn (u_{rms}^{2}) ——– (2)

Divided (2) by (1)

K.E / PV = 1/2 mn (u_{rms}^{2}) / 1/3 mn u_{rms}^{2}

K.E / PV = 3/2

K.E = 3/2 PV ——– (3)

As,

PV = nRT

For one mole of an ideal gas n=1

PV = RT

Put of the value of PV in (3)

**K.E = 3/2 RT** **(KE of one mole of an ideal gas)**

The most important thing is that the kinetic energy of the gas is independent of the nature of the gas. It only depends on the temperature.

As we know,

K.E of one mole of an ideal gas = 3/2 RT

For n moles of an ideal gas

**K.E of n moles of an ideal gas = 3/2 nRT**

As 1 mole = N_{A} molecules = 6.02×10^{23} molecules

K.E of one molecule = 3RT / 2N_{A}

Where R/N_{A} is Bolt’zmen constant (K)

**K.E of one molecule = 3/2 KT**

#### Note:

Basically, these derivatives are only true for monoatomic ideal gas. (Helium, Neon, Argon are monoatomic gases)

## Deduction of Gas Laws From the Kinetic Gas Equation

### 1. Boyle’s Law

According to the kinetic equation

PV = 1/3 mnu_{rms}^{2} or

PV = (2/3) × 1/2mnu_{rms}^{2} ——– (1)

Where,

- 1/2 mnu
_{rms}^{2}is the average kinetic energy of molecules.

According to the kinetic molecular theory of gases, the average kinetic energy of the molecule is directly proportional to the absolute temperature.

K.E ∝ T

1/2 mnu_{rms}^{2} ∝ T

1/2 mnu_{rms}^{2} = KT ——– (2)

From equation (1) and (2)

PV = 2/3 KT

At constant temperature, PV = K which is **Boyle’s Law**

### 2. Charles’s Law

As

PV = 2/3 KT

V = 2/3 KT/P

At constant pressure, 2/3 K/P is constant

Hence, V ∝ T which is **Charles’s Law**

### 3. Avogadro’s Law

As the kinetic equation of gas,

PV = 1/3 mnu_{rms}^{2}

For gas (1); P_{1}V_{1} = 1/3 m_{1}n_{1}u_{1rms}^{2}

For gas (2); P_{2}V_{2} = 1/3 m_{2}n_{2}u_{2}rms^{2}

If the pressure and volume of two gases are equal, then

1/3 m_{1}n_{1}u_{1rms}^{2} = 1/3 m_{2}n_{2}u_{2}rms^{2} ———- (3)

If two gases are at the same temperature, the average kinetic energy per molecule will be the same.

1/2 m_{1}u_{1}^{2} = 1/2 m_{2}u_{2}^{2} ——– (4)

Divided equation (3) by (4)

n_{1} = n_{2} which is **Avodagro’s Law.**

### 4. Graham’s Law of Diffusion

According to the kinetic gas equation,

PV = 1/3 mnu_{rms}^{2}

For one mole of gas n=N_{A}, we can write

PV = 1/3 mN_{A}u_{rms}^{2}

Where N_{A} is Avogadro’s number (mN_{A} = M)

PV = 1/3 Mu_{rms}^{2}

u_{rms}^{2} = 3PV/M = 3P/M/V = 3P/d (d=M/V)

or u_{rms}^{2} ∝ 1/d

u_{rms} ∝ √1/d

Now, “r” the rate of diffusion of the gas is directly proportional to the rms velocity of the molecules, thus

r ∝ √1/d which is **Graham’s law of diffusion.**

### 5. Daltan’s Law of Partial Pressure

If n_{1} molecules of a gas, each of mass m_{1} and velocity u_{1}, occupy a volume V, then pressure P exerted by these molecules is given by,

P_{1} = 1/3 m_{1}n_{1}u_{1rms}/V

Similarly, pressure P_{2} exerted by n_{2} molecules of another gas, each of mass m_{2} and velocity u_{2} is given by,

P_{2} = 1/3 m_{2}n_{2}u_{2rms}/V

In the same way, pressure P_{3} of a third gas is given by

P_{3} = 1/3 m_{3}n_{3}u_{3rms}/V

If all the three gases are kept together in another flask of the same volume and at the same temperature then total pressure P is given by,

P = P_{1} = 1/3 m_{1}n_{1}u_{1rms}/V + 1/3 m_{2}n_{2}u_{2rms}/V + 1/3 m_{3}n_{3}u_{3rms}/V

P = P_{1} + P_{2} + P_{3} which is **Dalton’s Law of partial pressure.**

## Numericals of Kinetic Equation

### Find the kinetic equation of 8g of methane at 27℃?

Temp = 27℃ = 27 + 273K = 300K

K.E_{(1 mole)} = 3/2 RT

For n moles,

K.E_{(n moles)} = 3/2 nRT

n = m/M = 8/16 = 0.5

K.E_{(n moles)} = 3/2 (0.5) × (8.314) × 300K

**K.E = 1870.65 J/mol**

### Find the change in kinetic energy of one mole of an ideal gas when temperature changes by 50℃?

K.E = 3/2 RT

Intial K.E = K.E_{i} = 3/2 RT

Final K.E = K.E_{f} = 3/2 R (T+50℃)

△K.E = Final – Intial

△K.E = 3/2 R (T+50℃) – 3/2 RT

△K.E = 3/2 R (T+50 – T)

△K.E = 3/2 R × 50

△K.E = 3/2 × 8.314 ×50

**△K.E = 610.05 J**

### At what temperature, the kinetic energy will be half of its value at 127℃?

Temp = 127℃ = 400K

K.E = 3/2 RT

K.E_{(127℃)} = 3/2 R × 400K

At what temperature “T” the kinetic energy will half

K.E_{(T)} = K.E_{(127℃) }/ 2

3/2 RT = 3/2 R × 400K / 2

T = 400/2

**T = 200K**

#### Another method:

K.E ∝ T

When the temperature is half, the kinetic energy will behalf

Given temp = 127℃ = 400K

K.E = 400K

Temperature becomes half 200K

**K.E/2 = 200k**

### We have a container containing 1 mole helium of molar mass of 4g. One size length (L) of container is 2cm and they make 500 collisions with the wall in each second. Find the temperature of gas?

As helium gas make 500 collisions in one second so,

Time for one second = 1/500 s ——– (1)

Time is taken for one collision = Distance / speed

Time is taken for one collision = 2L / u_{rms} ——– (2)

Compare (1) and (2)

1/500 = 2L / u_{rms}

1/500 = 2 × 2×10^{-2} / u_{ums}

u_{rms} = (2 × 2×10^{-2}) × (500)

u_{rms} = 20 m/s

K.E of one molecule = 1/2 mu_{rms}^{2} ——– (3)

K.E of one molecule = 3/2 KT ——– (4) where K=Bolt’zmen constant

Compare (3) and (4)

1/2 mu_{rms}^{2} = 3/2 KT

mu_{rms}^{2} = 3 KT

T = mu_{rms}^{2} / 3K ——– (5)

m is the number of molecules

Molar mass of one mole of He = 4g

mass of one molecule of He = 4 amu

As we know that 1 amu = 1.67×10^{-27}kg

m = 4 × 1.67×10^{-27}

K = 1.38×10^{-23} J/K (K is Bolt’zmen constant)

Putting all the values in (5)

T =4 × 1.67×10^{-27} × (20)^{2} / 3(1.38×10^{-23})

T = 2.672×10^{-24} / 4.414×10^{-23}

**T = 0.0515 K **